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Dynamics of signaling between Ca(2+) sparks and Ca(2+)- activated K(+) channels studied with a novel image-based method for direct intracellular measurement of ryanodine receptor Ca(2+) current

机译:Ca(2+)火花和Ca(2 +)激活的K(+)通道之间的信号动力学研究用一种新的基于图像的方法直接细胞内测量兰尼碱受体Ca(2+)电流

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摘要

Ca(2+) sparks are highly localized cytosolic Ca(2+) transients caused by a release of Ca(2+) from the sarcoplasmic reticulum via ryanodine receptors (RyRs); they are the elementary events underlying global changes in Ca(2+) in skeletal and cardiac muscle. In smooth muscle and some neurons, Ca(2+) sparks activate large conductance Ca(2+)-activated K(+) channels (BK channels) in the spark microdomain, causing spontaneous transient outward currents (STOCs) that regulate membrane potential and, hence, voltage-gated channels. Using the fluorescent Ca(2+) indicator fluo-3 and a high speed widefield digital imaging system, it was possible to capture the total increase in fluorescence (i.e., the signal mass) during a spark in smooth muscle cells, which is the first time such a direct approach has been used in any system. The signal mass is proportional to the total quantity of Ca(2+) released into the cytosol, and its rate of rise is proportional to the Ca(2+) current flowing through the RyRs during a spark (I(Ca(spark))). Thus, Ca(2+) currents through RyRs can be monitored inside the cell under physiological conditions. Since the magnitude of I(Ca(spark)) in different sparks varies more than fivefold, Ca(2+) sparks appear to be caused by the concerted opening of a number of RyRs. Sparks with the same underlying Ca(2+) current cause STOCs, whose amplitudes vary more than threefold, a finding that is best explained by variability in coupling ratio (i.e., the ratio of RyRs to BK channels in the spark microdomain). The time course of STOC decay is approximated by a single exponential that is independent of the magnitude of signal mass and has a time constant close to the value of the mean open time of the BK channels, suggesting that STOC decay reflects BK channel kinetics, rather than the time course of [Ca(2+)] decline at the membrane. Computer simulations were carried out to determine the spatiotemporal distribution of the Ca(2+) concentration resulting from the measured range of I(Ca(spark)). At the onset of a spark, the Ca(2+) concentration within 200 nm of the release site reaches a plateau or exceeds the [Ca(2+)](EC50) for the BK channels rapidly in comparison to the rate of rise of STOCs. These findings suggest a model in which the BK channels lie close to the release site and are exposed to a saturating [Ca(2+)] with the rise and fall of the STOCs determined by BK channel kinetics. The mechanism of signaling between RyRs and BK channels may provide a model for Ca(2+) action on a variety of molecular targets within cellular microdomains.
机译:Ca(2+)火花是高度局部的胞质Ca(2+)瞬变,是通过ryanodine受体(RyRs)从肌质网释放Ca(2+)引起的;它们是骨骼肌和心肌中Ca(2+)全局变化的基础基本事件。在平滑肌和某些神经元中,Ca(2+)火花激活火花微域中的大电导Ca(2+)激活的K(+)通道(BK通道),导致自发的瞬时向外电流(STOC),调节膜电位和,因此是电压门控通道。使用荧光Ca(2+)指示剂fluo-3和高速宽视场数字成像系统,可以捕获在平滑肌细胞中产生火花期间荧光的总增加量(即信号质量),这是第一个在任何系统中都曾使用过这种直接方法。信号质量与释放到细胞质中的Ca(2+)总量成正比,其上升速率与火花期间流过RyRs的Ca(2+)电流成比例(I(Ca(spark)) )。因此,可以在生理条件下在细胞内部监测通过RyRs的Ca(2+)电流。由于不同火花中I(Ca(spark))的大小变化超过五倍,因此Ca(2+)火花似乎是由许多RyR的一致打开引起的。具有相同底层Ca(2+)电流的火花会导致STOC,其幅度变化超过三倍,这一发现可以用耦合比(即火花微域中RyRs与BK通道的比)的变化来最好地解释。 STOC衰减的时间过程由单个指数来近似,该指数与信号质量的大小无关,并且其时间常数接近BK通道的平均打开时间的值,这表明STOC衰减反映了BK通道动力学,而不是比[Ca(2+)]在膜上下降的时间过程。进行计算机模拟以确定由I(Ca(spark))的测量范围导致的Ca(2+)浓度的时空分布。在发生火花时,与释放速率相比,释放部位200 nm内的Ca(2+)浓度达到平稳或超过BK通道的[Ca(2 +)](EC50)。 STOC。这些发现提出了一个模型,其中BK通道位于释放位置附近,并通过BK通道动力学确定STOC的上升和下降而暴露于饱和的[Ca(2+)]。 RyRs和BK通道之间的信号传导机制可能提供Ca(2+)作用于细胞微域内各种分子靶标的模型。

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